Determination of large strains in metalforming

1982 ◽  
Vol 17 (2) ◽  
pp. 95-101 ◽  
Author(s):  
R Sowerby ◽  
E Chu ◽  
J L Duncan

Certain techniques for the experimental determination of large strains in metalforming are discussed. The methods employ a grid pattern marked on the surface of the workpiece before forming and subsequently measured after deformation. The grid method is a surface phenomenon and the strain determination is reduced to a two dimensional problem. Any measurements taken on the initial and final grid configurations only, without knowing the deformation path, are insufficient to determine the strains precisely. Nevertheless, in practice, strains are determined by such a technique, often by using grid circles and by further assuming they deform into ellipses. The deformation process which transforms circles to ellipses and straight lines to straight lines, still does not define the straining path. Under such a deformation mode strain paths can be divided into two main types, those where an initially orthogonal pair of line elements (the principal axes) remain orthogonal throughout the deformation and those where they do not. The same change in shape can be achieved by either type of straining path, but the distinction between each straining mode is discussed and analysed in simple terms. The analysis is performed with reference to a square or quadrilateral grid of lines since automatic image analysis can be most effectively exploited when using coordinate or nodal point measures.

1966 ◽  
Vol 1 (3) ◽  
pp. 216-222 ◽  
Author(s):  
T. C. Hsu

In manufacturing processes involving large strains, the properties of the material undergoing deformation depend not only on the current total strain but on the previous strain path as well. Strain paths are divided into two major types, those in which the principal axes of strain remain fixed with respect to the material (coaxial strain paths), and those in which they rotate (non-coaxial strain paths). The characteristics of the two types of strain path are explained. Particular types of non-coaxial strain path related to practical applications are discussed in further detail and examples based on actual measurements are given.


1983 ◽  
Vol 18 (2) ◽  
pp. 119-123 ◽  
Author(s):  
R Sowerby ◽  
P C Chakravarti

This article considers the in-plane deformation of a thin, incompressible membrane undergoing an arbitrary, but finite, homogeneous deformation mode. No discontinuities in the loading system are permitted, and the nature of the straining process is assumed unchanged from beginning to end. For these restricted deformation modes a technique is described whereby the equivalent strain can be evaluated by measuring the initial and final shape only of a finitely deformed grid marked on the surface of the membrane. The analysis is performed with reference to an initially square or rectangular grid of lines, since the nodes of the grid facilitate the experimental measurements. A distinction is drawn between homogeneous deformation and the special case of pure homogeneous deformation which results in the same shape change. In the latter mode a pair of principal axes can be identified which remain orthogonal during the entire deformation history; while for the former mode there is no such line pair which preserves orthogonality throughout the deformation. The article concludes with a brief discussion on the determination of strain in industrial stampings.


2017 ◽  
Vol 40 (12) ◽  
pp. 3050-3060
Author(s):  
Yu Takahashi ◽  
Nicholas Bradley ◽  
Brian Kennedy

2019 ◽  
Vol 8 (1) ◽  
pp. 328-339
Author(s):  
P. Pramod Chakravarthy ◽  
Kamalesh Kumar

Abstract In this paper, a time dependent singularly perturbed differential-difference convection-diffusion equation is solved numerically by using an adaptive grid method. Similar boundary value problems arise in computational neuroscience in determination of the behaviour of a neuron to random synaptic inputs. The mesh is constructed adaptively by using the concept of entorpy function. In the proposed scheme, prior information of the width and position of the layers are not required. The method is independent of perturbation parameter ε and gives us an oscillation free solution, without any user introduced parameters. Numerical examples are presented to show the accuracy and efficiency of the proposed scheme.


The first study of meteoric iron by X-ray methods was undertaken at the instigation of Professor S. W. J. Smith, F.R.S. some years ago. This research (Young 1926) resulted not only in the determination of the crystal structures of two of the main constituents, kamacite and taenite, but also in the important discovery of the nature of the mutual orientations of these constituents when the meteorite exhibits a Widmanstätten structure. As is well known, the Widmanstätten figures in meteorites arise from the arrangement of kamacite lamellae on the planes of an octahedron, and for that reason a meteorite exhibiting these figures is generally referred to as an octahedrite. The kamacite lamellae, therefore, fix the {I I I}-planes of a hypothetical cubic lattice whose principal axes, XYZ , will be referred to as “ the axes of the octahedrite”.


2007 ◽  
Vol 344 ◽  
pp. 113-118 ◽  
Author(s):  
Massimo Tolazzi ◽  
Marion Merklein

This paper presents a method for the experimental determination of forming limit diagrams under non linear strain paths. The method consists in pre-forming the sheets under two different strain conditions: uniaxial and biaxial, and then stretching the samples, cut out of the preformed sheets, using a Nakajima testing setup. The optical deformation measurement system used for the process analysis (ARAMIS, Company GOM) allows to record and to analyze the strain distribution very precisely with respect to both time and space. As a reference also the FLDs of the investigated grades (the deep drawing steel DC04, the dual phase steel DP450 and the aluminum alloy AA5754) in as-received conditions were determined. The results show as expected an influence of the pre-forming conditions on the forming limit of the materials, with an increased formability in the case of biaxial stretching after uniaxial pre-forming and a reduced formability for uniaxial load after biaxial stretching if compared to the case of linear strain paths. These effects can be observed for all the investigated materials and can be also described in terms of a shifting of the FLD, which is related to the art and magnitude of the pre-deformation.


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